The maximum velocity divided by the average velocityin laminar poisseuille flow between two parallel plates is
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and velocity of laminar flow
garala brijesh -Posted on 25 Apr 16
Good
Pankaj -Posted on 29 Sep 15
• The equation of velocity distribution of laminar fluid flow through a pipe having radius R is given by,
u = – (1 / (4 μ)) (∂p/∂x) [R2 – r2]
where,
u = velocity of fluid
R = radius of pipe
r = distance from the centre of the pipe
• Maximum velocity occurs at the centre where r = 0. Putting this in above equation,
Umax = – (1 / (4 μ)) (∂p/∂x) [R2]
• Average velocity obtained by dividing discharge of the fluid across the cross sectional area of pipe (πR2)
dQ = Velocity at radus r x Area of ring element
= u x 2πr dr
= – (1 / (4 μ)) (∂p/∂x) [R2] x 2πr dr
• Therefore,
Q = 0∫R – (1 / (4 μ)) (∂p/∂x) [R2] x 2πr dr
= (π/8μ) (- ∂p/∂x) R4
• Therefore, Average velocity,
u = Q/A
u = (1/8μ) (- ∂p/∂x) R2
• Ratio of maximum and average velocity
Umax / u = 2
garala brijesh -Posted on 25 Apr 16
Good
Pankaj -Posted on 29 Sep 15
• The equation of velocity distribution of laminar fluid flow through a pipe having radius R is given by,
u = – (1 / (4 μ)) (∂p/∂x) [R2 – r2]
where,
u = velocity of fluid
R = radius of pipe
r = distance from the centre of the pipe
• Maximum velocity occurs at the centre where r = 0. Putting this in above equation,
Umax = – (1 / (4 μ)) (∂p/∂x) [R2]
• Average velocity obtained by dividing discharge of the fluid across the cross sectional area of pipe (πR2)
dQ = Velocity at radus r x Area of ring element
= u x 2πr dr
= – (1 / (4 μ)) (∂p/∂x) [R2] x 2πr dr
• Therefore,
Q = 0∫R – (1 / (4 μ)) (∂p/∂x) [R2] x 2πr dr
= (π/8μ) (- ∂p/∂x) R4
• Therefore, Average velocity,
u = Q/A
u = (1/8μ) (- ∂p/∂x) R2
• Ratio of maximum and average velocity
Umax / u = 2
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